Chapter 8 - 1
ISSUES TO ADDRESS...
• How do cracks that lead to failure form?
• How is fracture resistance quantified? How do the fracture
resistances of the different material classes compare?
• How do we estimate the stress to fracture?
• How do loading rate, loading history, and temperature
affect the failure behavior of materials?
Ship-cyclic loading
from waves.
Computer chip-cyclic
thermal loading.
Hip implant-cyclic
loading from walking.
Adapted from Fig. 22.30(b), Callister 7e. (Fig. 22.30(b) is courtesy of National Semiconductor Corporation.)
Adapted from Fig. 22.26(b), Callister 7e.
Chapter 8: Mechanical Failure
Adapted from chapter-opening photograph, Chapter 8, Callister & Rethwisch 8e. (by Neil Boenzi, The New York Times.)
Chapter 8 - 2
Fracture mechanisms
• Ductile fracture
– Accompanied by significant plastic
deformation
• Brittle fracture
– Little or no plastic deformation
– Catastrophic
Chapter 8 - 3
Ductile vs Brittle Failure
Very
Ductile
Moderately
Ductile
Brittle
Fracture
behavior:
Large
Moderate
%AR or %EL
Small
•
Ductile fracture is
usually more desirable
than brittle fracture!
Adapted from Fig. 8.1, Callister & Rethwisch 8e.
• Classification:
Ductile:
Warning before
fracture
Brittle:
No
warning
Chapter 8 - 4
•
Ductile
failure:
-- one piece
-- large deformation
Figures from V.J. Colangelo and F.A. Heiser, Analysis of Metallurgical Failures (2nd ed.), Fig. 4.1(a) and (b), p. 66 John Wiley and Sons, Inc., 1987. Used with permission.
Example: Pipe Failures
•
Brittle
failure:
-- many pieces
Chapter 8 - 5
• Resulting
fracture
surfaces
(steel)
50 mm
particles
serve as void
nucleation
sites.
50 mm
From V.J. Colangelo and F.A. Heiser, Analysis of Metallurgical Failures (2nd ed.), Fig. 11.28, p. 294, John Wiley and Sons, Inc., 1987. (Orig. source: P. Thornton, J. Mater. Sci., Vol. 6, 1971, pp. 347-56.)
100 mm
Fracture surface of tire cord wire loaded in tension. Courtesy of F. Roehrig, CC Technologies, Dublin, OH. Used with permission.
Moderately Ductile Failure
• Failure Stages:
necking
void
nucleation
void growth
and coalescence
shearing
at surface
fracture
Chapter 8 - 6
Moderately Ductile vs. Brittle Failure
Adapted from Fig. 8.3, Callister & Rethwisch 8e.
Chapter 8 - 7
Brittle Failure
Arrows indicate point at which failure originated
Chapter 8 - 8
•
Inter
granular
(
between
grains)
304 S. Steel
(metal)
Reprinted w/permission from "Metals Handbook", 9th ed, Fig. 633, p. 650. Copyright 1985, ASM International, Materials Park, OH. (Micrograph by J.R. Keiser and A.R. Olsen, Oak Ridge National Lab.)
Polypropylene
(polymer)
Reprinted w/ permission from R.W. Hertzberg, "Defor-mation and Fracture Mechanics of Engineering Materials", (4th ed.) Fig. 7.35(d), p. 303, John Wiley and Sons, Inc., 1996.4
mm
•
Trans
granular
(
through
grains)
Al Oxide
(ceramic)
Reprinted w/ permission from "Failure Analysis of Brittle Materials", p. 78. Copyright 1990, The American Ceramic Society, Westerville, OH. (Micrograph by R.M. Gruver and H. Kirchner.)316 S. Steel
(metal)
Reprinted w/ permission from "Metals Handbook", 9th ed, Fig. 650, p. 357. Copyright 1985, ASM International, Materials Park, OH. (Micrograph by D.R. Diercks, Argonne National Lab.)
3
mm
160
mm
1
mm
(Orig. source: K. Friedrick, Fracture 1977, Vol. 3, ICF4, Waterloo, CA, 1977, p. 1119.)
Chapter 8 - 9
• Stress-strain behavior (Room T):
Ideal vs Real Materials
TS << TS
engineering
materials
perfect
materials
E/10
E/100
0.1
perfect mat’l-no flaws
carefully produced glass fiber
typical ceramic
typical strengthened metal
typical polymer
• DaVinci (500 yrs ago!) observed...
-- the longer the wire, the
smaller the load for failure.
• Reasons:
-- flaws cause premature failure.
-- larger samples contain longer flaws!
Reprinted w/ permission from R.W. Hertzberg, "Deformation and Fracture Mechanics of Engineering Materials", (4th ed.) Fig. 7.4. John Wiley and Sons, Inc., 1996.
Chapter 8 - 10
Flaws are Stress Concentrators!
• Griffith Crack
where
t
= radius of curvature
o= applied stress
m
= stress at crack tip
a
= lenght of crack
K
t= Stress concentration factor
(
m/
o)
t
Adapted from Fig. 8.8(a), Callister & Rethwisch 8e.
o
t
t
o
m
K
2
/
1
2
a
Chapter 8 - 11
Concentration of Stress at Crack Tip
Adapted from Fig. 8.8(b), Callister & Rethwisch 8e.
Chapter 8 - 12
Crack Creation & Propagation
Cracks having sharp tips propagate
easier than cracks having blunt tips
deformed
region
brittle
Energy balance on the crack
• Elastic strain energy-
• energy stored in material as it is elastically deformed
• this energy is released when the crack propagates
• creation of new surfaces requires energy
ductile
• Avoid sharp corners!
r ,
fillet
radius
w
h
max
Chapter 8 - 13
Criterion for Crack Propagation
Crack propagates if crack-tip stress (
m
)
exceeds a
critical stress
(
c
)
where
– E = modulus of elasticity
–
s= specific surface energy
– a = one half length of internal crack
For ductile materials => replace
s
with
s
+
p
where
p
is plastic deformation energy
2
/
1
2
a
s
c
E
i.e.,
m
>
c
Chapter 8 - 14
• Crack growth condition:
•
Largest
, most highly
stressed
cracks grow first!
Design Against Crack Growth
K
Ic
=
Y
a
--Scenario 1:
Max. flaw
size dictates design stress.
max
a
Y
K
Ic
design
a
max
no
fracture
fracture
--Scenario 2:
Design stress
dictates max. flaw size.
2
max
1
design
Ic
Y
K
a
a
max
no
fracture
fracture
K
c
= Fracture toughness
Chapter 8 - 15
Design Example: Aircraft Wing
Answer:
(
c
)
B
168
MPa
• Two designs to consider...
Design A
--largest flaw is 9 mm
--failure stress = 112 MPa
Design B
--use same material
--largest flaw is 4 mm
--failure stress = ?
• Key point: Y and K
Ic
are the same for both designs.
• Material has K
Ic
= 26 MPa-m
0.5
• Use...
max
a
Y
K
Ic
c
B
max
A
max
a
a
c
c
9 mm
112 MPa
4 mm
--Result:
=
a
=
Y
K
Ic
constant
Chapter 8 - 16
Impact Testing
final height
initial height
• Impact loading:
-- severe testing case
-- makes material more brittle
-- decreases toughness
Adapted from Fig. 8.12(b), Callister & Rethwisch 8e. (Fig. 8.12(b) is adapted from H.W. Hayden, W.G. Moffatt, and J. Wulff, The Structure and
Properties of Materials, Vol. III, Mechanical Behavior, John Wiley and Sons, Inc. (1965) p. 13.)
Chapter 8 - 17
Influence of Temperature on
Impact Energy
Adapted from Fig. 8.15, Callister & Rethwisch 8e.
•
Ductile-to-Brittle Transition Temperature (DBTT)
...
BCC metals (e.g., iron at T < 914ºC)
Im
pac
t
Energy
Temperature
High strength materials (
y
> E/150)
polymers
More Ductile
Brittle
Ductile-to-brittle
transition temperature
Chapter 8 - 18
• Pre-WWII: The Titanic
• WWII: Liberty ships
• Problem: Steels were used having DBTT’s just below
room temperature
.
Reprinted w/ permission from R.W. Hertzberg,
"Deformation and Fracture Mechanics of Engineering Materials", (4th ed.) Fig. 7.1(a), p. 262, John Wiley and Sons, Inc., 1996. (Orig. source: Dr. Robert D. Ballard, The Discovery of the Titanic.)
Reprinted w/ permission from R.W. Hertzberg,
"Deformation and Fracture Mechanics of Engineering Materials", (4th ed.) Fig. 7.1(b), p. 262, John Wiley and Sons, Inc., 1996. (Orig. source: Earl R. Parker,
"Behavior of Engineering Structures", Nat. Acad. Sci., Nat. Res. Council, John Wiley and Sons, Inc., NY, 1957.)
Design Strategy:
Chapter 8 - 19
Fatigue
Adapted from Fig. 8.18, Callister & Rethwisch 8e. (Fig. 8.18 is from Materials Science in Engineering, 4/E by Carl. A. Keyser, Pearson Education, Inc., Upper Saddle River, NJ.)
•
Fatigue
= failure under applied cyclic stress.
• Stress varies with time.
-- key parameters are
S
,
m
, and
cycling frequency
max
min
time
m
S
• Key points: Fatigue...
--can cause part failure, even though
max
<
y
.
--responsible for ~ 90% of mechanical engineering failures.
tension on bottom
compression on top
counter
motor
flex coupling
specimen
bearing
bearing
Chapter 8 - 20 Adapted from Fig. 8.19(a), Callister & Rethwisch 8e.
Types of Fatigue Behavior
•
Fatigue limit
,
S
fat
:
--no fatigue if S < S
fat
S
fatcase for
steel
(typ.)
N = Cycles to failure
10
3
10
5
10
7
10
9
unsafe
safe
S
=
s
tress
ampl
itude
• For some materials,
there is no fatigue
limit!
Adapted from Fig. 8.19(b), Callister & Rethwisch 8e.
case for
Al
(typ.)
N = Cycles to failure
10
3
10
5
10
7
10
9
unsafe
safe
S
=
s
tress
ampl
itude
Chapter 8 - 21
• Crack grows incrementally
typ. 1 to 6
a
~
increase in crack length per loading cycle
• Failed rotating shaft
-- crack grew even though
K
max
< K
c
-- crack grows faster as
•
increases
• crack gets longer
• loading freq. increases.
crack origin
Adapted from
Fig. 8.21, Callister & Rethwisch 8e. (Fig. 8.21 is from D.J. Wulpi, Understanding How Components Fail, American Society for Metals, Materials Park, OH, 1985.)
Rate of Fatigue Crack Growth
m
K
dN
Chapter 8 - 22
Improving Fatigue Life
2. Remove stress
concentrators.
Adapted fromFig. 8.25, Callister & Rethwisch 8e.
bad
bad
better
better
Adapted fromFig. 8.24, Callister & Rethwisch 8e.
1. Impose compressive
surface stresses
(to suppress surface
cracks from growing)
N = Cycles to failure
moderate tensile
m
Larger tensile
m
S
=
s
tre
s
s
ampli
tude
near zero or compressive
m
--Method 1: shot peening
put
surface
into
compression
shot
--Method 2: carburizing
Chapter 8 - 23
Creep
Sample deformation at a constant stress ( ) vs. time
Adapted from
Fig. 8.28, Callister & Rethwisch 8e.
Primary Creep: slope (creep rate)
decreases with time.
Secondary Creep
: steady-state
i.e., constant slope
/ t)
Tertiary Creep: slope (creep rate)
increases with time, i.e. acceleration of rate.
Chapter 8 - 24
• Occurs at elevated temperature, T > 0.4 T
m
(in K)
Adapted from Fig. 8.29, Callister & Rethwisch 8e.
Creep: Temperature Dependence
elastic
primary
secondary
Chapter 8 - 25
Secondary Creep
• Strain rate is constant at a given T,
-- strain hardening is balanced by recovery
stress exponent (material parameter)
strain rate
activation energy for creep
(material parameter)
applied stress
material const.
• Strain rate
increases
with increasing
T,
10
2
0
4
0
10
0
2
0
0
10
-2
10
-1
1
Steady state creep rate (%/1000hr)
s
St
re
ss
(MPa)
427ºC
538ºC
649ºC
Adapted fromFig. 8.31, Callister 7e. (Fig. 8.31 is from Metals Handbook: Properties and Selection:
Stainless Steels, Tool Materials, and Special Purpose Metals, Vol. 3, 9th ed., D. Benjamin (Senior Ed.), American Society for Metals, 1980, p. 131.)
RT
Q
K
n
c
s
2
exp
Chapter 8 -
Creep Failure
• Failure:
along grain boundaries.
applied
stress
g.b. cavities
From V.J. Colangelo and F.A. Heiser, Analysis of Metallurgical Failures (2nd ed.), Fig. 4.32, p. 87, John Wiley and Sons, Inc., 1987. (Orig. source: Pergamon Press, Inc.)
Chapter 8 - 27